Surface aggregation patterns of LDL receptors near coated pits III: potential effects of combined retrograde membrane flow-diffusion and a polarized-insertion mechanism
© Echavarria-Heras et al.; licensee BioMed Central Ltd. 2014
Received: 26 November 2013
Accepted: 12 May 2014
Published: 22 May 2014
Although the process of endocytosis of the low density lipoprotein (LDL) macromolecule and its receptor have been the subject of intense experimental research and modeling, there are still conflicting hypotheses and even conflicting data regarding the way receptors are transported to coated pits, the manner by which receptors are inserted before they aggregate in coated pits, and the display of receptors on the cell surface. At first it was considered that LDL receptors in human fibroblasts are inserted at random locations and then transported by diffusion toward coated pits. But experiments have not ruled out the possibility that the true rate of accumulation of LDL receptors in coated pits might be faster than predicted on the basis of pure diffusion and uniform reinsertion over the entire cell surface. It has been claimed that recycled LDL receptors are inserted preferentially in regions where coated pits form, with display occurring predominantly as groups of loosely associated units. Another mechanism that has been proposed by experimental cell biologists which might affect the accumulation of receptors in coated pits is a retrograde membrane flow. This is essentially linked to a polarized receptor insertion mode and also to the capping phenomenon, characterized by the formation of large patches of proteins that passively flow away from the regions of membrane exocytosis. In this contribution we calculate the mean travel time of LDL receptors to coated pits as determined by the ratio of flow strength to diffusion-coefficient, as well as by polarized-receptor insertion. We also project the resulting display of unbound receptors on the cell membrane. We found forms of polarized insertion that could potentially reduce the mean capture time of LDL receptors by coated pits which is controlled by diffusion and uniform insertion. Our results show that, in spite of its efficiency as a possible device for enhancement of the rate of receptor trapping, polarized insertion nevertheless fails to induce the formation of steady-state clusters of receptor on the cell membrane. Moreover, for appropriate values of the flow strength-diffusion ratio, the predicted steady-state distribution of receptors on the surface was found to be consistent with the phenomenon of capping.
KeywordsLDL receptor dynamics Polarized receptor reinsertion Retrograde-flow model Mean capture time Surface-display capping
Endocytosis generally refers to the process by which substances are internalized through the cell membrane. Receptor-mediated endocytosis (RME) is a highly specialized kind of endocytosis in which large protein molecules called receptors project from the cell membrane and couple selectively to ligands such as low density lipoproteins (LDL) . Coated pits and their associated receptors have been studied most extensively in cells grown in culture, and the LDL receptor is the one on which a majority of experimental research has been conducted. The ligand-receptor complexes aggregate in specialized cell-membrane formations called coated pits [2–5]. When these close, they form vesicles which then transport the ligand-receptor complexes to the interior of the cell. Once the ligand-receptor bindings are separated, the ligands are degraded at the lysosomes. In some experimental systems, including the LDL system, the receptors are returned to the cell surface for further endocytic cycles, and the ligands are degraded at the lysosomes. Experimental results reveal that RME occurs in virtually all eukaryotic cells except the mature erythrocyte  and that it also provides an entrance mechanism for cell nutrients such as low density lipoproteins (LDL) , hormones and growth factors , serum transport proteins and antibodies , as well as toxins and lectins  and even viruses .
The low density lipoprotein (LDL) particles are cholesterol-transporting macromolecules that are produced in the liver and circulate in the plasma. Membrane reconstitution in human fibroblasts requires the assimilation of cholesterol. The efficiency of this process depends on the rate of endocytosis of the LDL macromolecule and its receptor. It is thought  that a severely depleted number of LDL receptors promotes high levels of circulating cholesterol because LDL internalization requires the receptor-binding stage. Deficiencies in the LDL cycle are known to be responsible for the ailment known as familial hypercholesterolemia, which promotes atherosclerosis and the incidence of strokes and coronary disease ; this being the reason why so much experimental research has been conducted on the internalization of the LDL receptor. A substantial portion of research aimed at the elucidation of the cholesterol-uptake process has addressed the characterization of the dynamics and display of the LDL receptor. This has produced a large pool of data and a sound conceptual framework which sustains the theoretical exploration of aspects of the dynamics mentioned above.
It is generally thought that the maintenance of receptors on the cell surface is due primarily to receptor recycling rather that to de novo synthesis. These data come from experiments using cycloheximide to block protein synthesis. In this experimental setup, it is observed that the number of LDL receptors on the cell surface remain roughly constant for at least six hours . Evidence of receptor internalization and reinsertion in unblocked systems would sustain the assumption that a steady-state concentration of receptors is maintained at the cell surface. The time receptors spend in the interior of the cell is negligible. The basis of this claim is the apparently undetectable pool of receptors inside the cell during endocytosis . The transit time for an LDL receptor from binding on coated pits to reappearance in the membrane, and found it to be on the order of 15 seconds . Based on these ideas, we will abide by the assumption that internalization and recycling of LDL receptors in human fibroblastic cells maintains the surface concentration of LDL at a steady state. Moreover, coated pits include 1% of the cell surface (coated pits include 2% of the cell surface at 4°C [15, 16], but when the temperature is raised to 37°C the number of coated pits on the surface is halved ). Anderson et al.  assert that coated pits tend to be linearly aligned over intracellular fibers. Hence, it can be assumed that the geometrical arrangement of coated pits on the cell surface of human fibroblasts can be reasonably approximated by means of a dilute and ordered system of sinks distributed on a two dimensional surface . Guadorov et al.  reported that coated pits tend to form repeatedly at defined sites while other regions are excluded. Therefore, we can assume that coated pits are infinitely long-lived traps distributed in a dilute and ordered form over the cell surface.
where ρ is the number of coated pits distributed per unit area on the cell surface.
Goldstein et al.  assert that whether traps are ordered or disordered makes only a small difference in the rate at which a trap captures receptors, given that the traps are distributed over the entire surface of the cell in a dilute way. Goldstein et al. [21, 25] dealt with two conflicting hypotheses about the coated-pit recycling process. In either case, the coated pit effectively has a finite lifetime. However, they found that the model of equations (6)-(12) obtained under the assumption that sinks have infinite lifetimes give good approximations for k d + in the experimental system for receptors of low density lipoproteins on human fibroblastic cells. Nevertheless, they also concluded that the experiments do not rule out the possibility that the true rate of accumulation of LDL receptors in coated pits could be faster than predicted on the basis of pure diffusion and uniform reinsertion all over the cell surface. A mechanism that has been proposed by experimental cell biologists which might affect the accumulation of receptors in coated pits is convection. Evidence of a membrane flow comes from the observation that, when the leading edge of a moving cell comes in contact with a small particle, the particle often adheres to the cell surface and is transported backward [26–28]. The motion of such adherent particles is consistent with particles undergoing Brownian motion in the presence of a constant membrane flow [29, 30]. It has been hypothesized that this flow originates when membrane components like specific receptors and lipids, which had been internalized from the cell surface, are recycled to the leading edge and contribute to the extension of the cell boundary . Considering that a rapid rate of membrane internalization is observed in endocytosis, a significant amount of recycled membrane should be made available for delivery at the leading edge. This delivery would be restricted to just those molecules that are internalized by coated pits [14, 31, 32], thus initiating the transport of membrane components away from the leading edge and towards the rear of the cell [26–31]. In addition to the specific delivery of receptors at the leading edge of the cell, their sorting within specific targets along the endocytic pathway have been proposed as components of a mechanism for the control of the internalization of specific ligands [18, 33–35]. Generally, eukaryotic cells show the ability to efficiently control the traffic of many types of macromolecules, targeting proteins and lipids for a variety of destinations, based on their types and the current needs of the cell. This traffic control is crucial for the maintenance of cellular structure and function [36, 37]. This makes it reasonable to assume that reinsertion of LDL receptors could be arranged in such a way that their trapping rate might be adapted to suit specific metabolic requirements. Moreover, it has been claimed  that in giant HeLa cells, receptors are not inserted uniformly into the plasma membrane but rather at the periphery of the cell. Robenek and Hesz  claimed that their experiments with LDL particles bound to colloidal gold provided the first clear demonstration of the sequential clustering of receptors near coated pits in plaques or loosely associated groups, and not in the form of widely dispersed individual units. They concluded that this effect is produced when recycled LDL receptors are inserted preferentially in membrane regions where coated pits form. According to Wofsy et al.  plaques could be conceptualized as receptor clusters surrounding coated pits. The idea of a retrograde flow is essentially connected to the concept of a polarized reinsertion of receptors. However, neither the influence of this insertion mode on the aggregation rate of LDL receptors in coated pits, nor the resultant steady-state surface aggregation patterns have been formally studied.
For the aims of the present research we extend the formal framework presented in Echavarria-Heras et al.  for the purpose of including diffusion aided by a retrograde flow, plus polarized receptor insertion as a combination of mechanisms that influences both the mean capture time τ du and the surface aggregation patterns of unbound LDL receptors. First, we conceptualize a partitioned receptor-insertion mode in which the cell membrane is divided into disjoint regions, each one receiving a fraction of the total number of recycled receptors. In the general form of this mode, different numbers of receptors are projected over the different regions partitioning the cell surface. Polarized insertion, moreover, corresponds to the case in which receptors are recycled into two disjoint regions having abruptly contrasting rates. This partitioned mode can be used to obtain arrangements—which can be seen as special cases—comprising uniform , locally uniform, peripheral , and plaque forms [39, 40], as well as a generalized radially symmetric mode of the form described in .
Different forms of the partitioned insertion rate function S rθ (c, p, p, m, α) : c , p and q stand for positive constants
Mode defining conditions
S rθ (c, 0, 0, b/a, 0)
S rθ (0, c, c, m, π)
S rθ (c, c, c, m, α)
S rθ (c, p, q, m, α)
S rθ (0, p, q, m, π)
S rθ (0, 0, q, m, π)
S rθ (0, p, 0, m, π)
S rθ (0, p, 0, m, α)
S rθ (0, p, q, m, α)
S rθ (0, 0, q, m, α)
For particular characterizations of S rθ (c, p, q, m, α), the resulting patterns of receptors can be simulated. These representations can be obtained by means of the computer graphics technique of ray tracing  using grey tones corresponding to the values of C λmα (r, θ).
Results and discussion
Anderson et al.  proposed that LDL receptors in human fibroblasts are inserted at random locations and are transported by diffusion toward coated pits, and Goldstein et al. [21, 25] have studied theoretical aspects of the dynamics of the LDL receptor on the cell surface. One of the questions addressed in these models was whether or not the random insertion of LDL receptors into the plasma membrane, followed by pure diffusion and using the measured diffusion coefficient for LDL receptors, could give a rapid enough aggregation of receptors in coated pits to account for the observed rate of removal of LDL from the cell surface. Since an experimentally determined lower bound for the forward rate constant k du + is (2.3 × 10- 10 ± 1.6) × 10- 10 cm 2/s and the value obtained from their model is 1.9 × 10- 10 cm 2/s, the answer to that question is that the hypothesis of random insertion and pure diffusion of LDL receptors to coated pits is consistent with experimental observations but just barely. Therefore, even though the diffusion-limited forward-rate constant k du + calculated by these authors is consistent with available experimental results on the rate of LDL internalization, these do not rule out the possibility that the true value of the mean capture time of receptors is actually smaller than τ du , the value predicted on the basis of random insertion of receptors followed by pure diffusion to coated pits. Indeed, if LDL receptors on human fibroblasts are not inserted uniformly into the plasma membrane, but are inserted preferentially into specialized regions where coated pits form, and if the resulting reduction in the time required for LDL receptors to diffuse to coated pits was significant, the conclusion that diffusion of LDL receptors to coated pits is the limiting step in the interaction of cell surface LDL receptors with coated pits could be wrong. Also, diffusion could be aided by a more active transport in order to increase the rate of accumulation of receptors in coated pits. In particular, we have studied here the effects of a polarized insertion of receptors as well as those related to a transport mechanism set by diffusion aided by a retrograde membrane flow.
Experimentally determined values for coated pit radius a and the outer radius b of the reference region Ω are respectively a = 0.10 ± 0.05 μm  and b = 1.0 ± 0.2 μm; these were obtained by using equation (5) with the calculated value for the suitable density of coated pits ρ = 0.31 ± 0.09/μm 2 . In order to typify values of the fundamental ratio λ = v/2D (cf. Eq. B1) we will use a low reference value v = v 0 for the strength v of the retrograde membrane flow. The value v 0 = 9.6 × 10- 7 cm/min represents the maximum of a hypothetical local flow that originates when coated pits invaginate to internalize the trapped ligand-receptor complexes . As a second reference value for the strength v of the retrograde flow we may take v 1 = 10- 4 cm/min. This value gives the approximate rate at which objects on the surface of fibroblasts are swept backwards [26, 14]. Since v 1 is approximately equal to 100v 0, this retrograde membrane-flow rate would sustain an extremely fast convective transport in comparison with one having a strength v 0. In order to characterize a variation range for the diffusion coefficient D, we will consider a normal process for the LDL receptor. This is associated with a diffusion coefficient value of D 0 = (2.7 ± 0.09) × 10- 9 cm2/min, which was determined by Barak and Webb  using fluorescence photo bleaching recovery (FBR) in an experimental arrangement involving LDL receptors diffusing on the surface of human fibroblast cells. We can also contemplate a fast diffusion process corresponding to D 1 = 8.1 × 10- 8 cm2/min, this being the average of the values defining the observed range of variation for the diffusion coefficient of the dil (3)- LDL receptor complex on blebs induced in the cell membrane. And we could also consider an extreme reference value of D ext = 6 × 10- 7 cm 2/min, that is D ext = 7.40D 1.
The phenomenon of capping is characterized by the formation of large patches of proteins that passively flow away from the regions of membrane exocytosis. Individual proteins can overcome this convective transport when they have diffusion coefficients (D) of about D ext . Moreover, a value for D of D ext /6 is comparable to the largest estimation for the diffusion coefficient of the dil (3)- LDL receptor complex on blebs . For the parameter values of the LDL system on human fibroblasts, the calculated value for τ du , the mean capture time when receptors move by pure diffusion and are inserted uniformly over the entire cell surface, is τ du = 2.92 min (cf. Eq. (11)).
If we now assume that λ = v 1/2D 0, that is, a relatively fast convective transport (v = v 1) and a normal diffusion process (D = D 0), and if we again choose the q-polarized insertion mode S rθ (0, 0, 1, 2, π/6 ) described above, then we will get τ λmα = 0.83 τ du . This result endorses the view that whenever convection becomes a relatively more active transport than diffusion, the process will fail to induce an effective randomization in the surface distribution of receptors . The relative dominance of convection over diffusion implies that those receptors favorably distributed in an area determined by the cross section of the coated pit perpendicular to flow streamlines could be trapped, while the others would be swept away by the flow. Therefore, whenever convection is relatively fast (v = v 1) we may assume that increasing D, that is, taking D > D 0 could induce relatively greater aggregation rates in coated pits. But since we have D 0 = (2.7 ± 0.09) × 10- 9 cm2/min, then the largest feasible experimentally determined value for D 0 is only D = 2.7910- 9 cm2/min, and this along with the S rθ (0, 0, 1, 2, π/6 ) mode and a fast convective transport will produce τ λmα = 0.75 τ du , which only amounts to a moderate reduction of the value τ λmα = 0.83 τ du calculated above. Further, if convection is relatively fast (v = v 1) and we still have a q-polarized insertion mode S rθ (0, 0, 1, 2, π/6 ), then unless we have D = 1.74D 0, the calculated value τ λmα will be significantly reduced: for that arrangement we obtained τ λmα = 0.24 τ du . Therefore, whenever convection is relatively fast (v = v 1), even for an efficient insertion mode such as the q-polarized form S rθ (0, 0, 1, 2, π/6), larger values than D = 1.74D 0 will be required for a noticeable reduction in τ du . Indeed, for a fast retrograde flow (v = v 1) and a fast diffusion process (D = D 1), we found that S rθ (0, 0, 1, 2, π/6 ) can produce a value of τ λmα = 0.01τ du , which is a drastic reduction of τ du . If we assume, moreover that receptors are returned to the cell surface through a p-polarized insertion mode with 0 < α ≤ π and with 9.5 ≤ m ≤ b/a, then even if convection is extremely fast (v = 300v 1), letting D = D ext , we get 0.19τ du ≤ τ λmα ≤ 0.65τ du . Compared with the results obtained above for the same insertion mode, this last inequality highlights the importance of diffusion in the reduction of the mean capture time of LDL receptors by coated pits. However, comparing with the expected variation range for D 0, D values beyond D = 2.7910- 8 cm2/min seem to be extremely high, and likely not achievable in the experimental system analyzed. Thus, before a faster diffusion process can be raised as an agent that can induce an effective randomization of the surface distribution of LDL receptors in the presence of a fast retrograde membrane flow, we assume instead that there must be another factor that could be adduced as a feasible device for promoting higher aggregation rates of LDL receptors in coated pits. And so, in accordance with the results presented here, we can suggest special forms of the insertion rate function S rθ (c, p, q, m, α) as mechanisms that potentially could boost the rate of removal of receptors by coated pits. Thus under the assumption of a fast convective transport, v = v 1, and a normal diffusion process, if we allow returning receptors to be sorted by means of a q-polarized insertion form by setting m = 1.3 and α = π/2, we would get τ λmα = 0.23τ du , implying a noticeable reduction in τ du . This means that whenever convection is fast and receptors diffuse normally, increasing the receptor-trapping rate could depend decidedly on polarized receptor insertion at preferential regions near coated pits.
Our results are mainly consistent with the capping phenomenon, and suggest that this is indeed concomitant with the idea of a retrograde membrane flow. Capping is described as the rearward transport across the leading lamella of various materials used to mark the cell surface [46, 14]. Bretscher  asserts that during capping, those receptors that are excluded by coated pits, and therefore do not recycle, may be continuously swept by a retrograde membrane flow. This author also states that whether such a non-circulating protein does get swept backwards or not depends on how fast it can diffuse by Brownian motion and how fast the flow is; and moreover that for individual proteins to overcome the sweeping effect of the flow, they must have diffusion coefficients (D) of about D ext . This assertion was corroborated by our results, since our model predicts that for D values of the order of D ext the capping effect can be reversed. Nevertheless, a value of D ext lies far beyond the maximum experimentally feasible value for D 0. And even though Bretscher  claims that FBR often underestimates the true value of the diffusion coefficients of pertinent surface receptors, a value D ext for D in the LDL experimental system seems unfeasible. Our results suggest that this is where the relative importance of non-uniform insertion becomes evident as a factor for boosting LDL receptor trapping. Indeed, even when convection is fast and receptors diffuse normally, our findings indicate that special forms of polarized receptor insertion can be arranged so as to produce a substantial reduction in τ du . This was more obvious in the case of a q-polarized mode, which could be raised as a feasible preferential-insertion mechanism for enhancing the LDL receptor trapping rate.
The problem of the surface distribution of unbound receptors is an important question pertaining to the LDL experimental system. For example, Wofsy et al.  argued that in the Robenek and Hesz  experiments, the LDL-gold particles were highly multivalent and thus may have been bound more efficiently to aggregate than single receptors, suggesting that the aggregation of newly inserted LDL receptors in regions around coated pits was still unproven. But beyond the caveats of Wofsy et al.  the results of Gross and Webb  were considered to provide a quantitative basis in support of a surface distribution of both LDL particles and their receptors in different-sized clusters. And again, the existence of these clusters was questioned by Sanan et al.  who reported experimental results that detected a dispersed or scattered population of LDL receptors, in addition to and clearly distinct from, clusters that formed soon after their insertion during recycling. In view of these disparate reports, Robenek et al.  performed new experiments on fibroblast and hepatocyte plasma membranes which confirmed their original claim that the initial insertion and display of LDL receptors in fibroblasts occurs predominantly as plaques. But experiments using fluorescently labeled LDL and influenza virus particles bound to the surface of human fibroblasts imaged with a cooled-scan CCD camera attached to a fluorescence microscope were found to yield a reasonably accurate measure of the proportion of single particles, but large errors were encountered in the proportion of large cluster sizes . The high proportion of single particles found in these data provided evidence against the clusters claimed by Robenek et al.  and support the random insertion model. It is still a matter of disagreement among different research groups whether newly inserted LDL receptors are dispersed in the plasma membrane of cultured fibroblasts prior to entrapment in coated pits or whether they remain after reinsertion as groups of clusters. Our findings reveal that in the presence of a fast retrograde membrane flow, the expected surface display of unbound receptors must be consistent with the capping phenomenon; thus, the formation of steady-state surface clumps of LDL receptors is unachievable in the current setting (Figure 12).
Traditionally the existence of a retrograde flow has been a source of controversy among researchers, some of whom disclaim this paradigm (e.g. [51–53]) while others convincingly address it (e.g. [14, 54, 55]). In particular, our results provide a theoretical support for the claim of Bretscher  which suggests that, if a retrograde flow does exist, the diffusion-convection ratio could be a fundamental determinant of the surface display of LDL receptors that are not bound to coated pits. And even though biochemical or biomechanical factors have been invoked in order to put forward other paradigms for the capping phenomenon (e.g. [49, 56–58]), our findings support the views of Bretscher  and Ishihara et al.  on the adequacy of the retrograde-flow model. Hence, the involvement of diffusion, polarized reinsertion and a retrograde membrane flow in the formalization of the receptor-mediated endocytic cycle may provide a trustworthy paradigm for the interpretation of observations. Moreover, the fact that some characterizations of the retrograde flow-diffusion ratio could induce slower receptor trapping rates cannot provide a rebuttal for the retrograde-flow model. Indeed, Echavarria-Heras et al.  suggested that receptors could be projected to the plasma membrane in a preferential mode relative to the flow streamlines. We have studied here the consequences of such an arrangement and our results show that certainly, even in the presence of a fast retrograde flow, we could consider a q-polarized form as a mechanism for the enhancement of LDL receptor trapping rates.
Our results seem to indicate that even in the presence of a fast retrograde membrane flow, which could influence capping-like effects, diffusing LDL receptors that are sorted through polarized insertion in the form conceptualized here, could spur faster aggregation rates in coated pits than those associated with uniform insertion over the entire cell membrane. Moreover a q-polarized form could provide a paradigm for a highly efficient form of preferential insertion. The effectiveness of this mode is mainly explained by its placement relative to the flow streamlines. Furthermore, if the cross sections of the linked insertion region Ω q (m, α) and those associated with a coated pit are comparable, then even though a relative dominance of convection over diffusion might occur, the privileged position of the insertion region Ω q (m, α) would induce a fast receptor-trapping rate. But our results also hint that in spite of the efficiency of this device, the influence of a retrograde flow would cancel out the display of the corresponding surface clusters. Moreover, if new experiments do reveal that the surface clusters exist, then it could be necessary to envision a mechanism that explains their formation in the presence of a retrograde membrane flow. Meanwhile, for the case v = v 1 and D = D 0, a q-polarized insertion mode with m = 1.20 and α = π/16 provides a convenient paradigm for explaining the coexistence of a retrograde membrane flow and receptor aggregations that might be experimentally misinterpreted as surface clusters. Indeed, considering the experimental error associated with the measurement of the coated pit radius, a region of insertion of the form Ω q with m = 1.20 could actually be a region placed over the boundary of a coated pit. And the surface clusters observed might be formed when recycling receptors are returned near the periphery of newly-formed coated pits so as to enhance the removal of the LDL ligand, but the existence of that insertion paradigm would require experimental substantiation.
The case in which receptors are inserted into two disjoint regions of abruptly contrasting rates is defined as a polarized insertion mode. It will be typified here as a mode that sorts the total number of recycled receptors over either the region Ω p (m, α), or Ω q (m, α), or Ω p (m, α) ∪ Ω q (m, α). Moreover, a polarized insertion mode can be obtained in five different forms, two of these forms being radially symmetric.
The function S rθ (0, 0, q, m, π) moreover, coincides with the plaque form insertion mode proposed by Wofsy et al. . And, by setting S rθ (0, 0, q, m, π) = Sr - β one obtains from equation (17) the decreasing and radially symmetric insertion-rate function considered by Echavarria-Heras et al. .
Where ∂Ωb denotes the outer boundary of the annulus Ω, since we have assumed a steady-state for the receptors. This requirement for a vanishing flux of particles across the boundary at r = b can be considered a model for a dynamics in which those receptors crossing the boundary at r = b are transported into a contiguous influence area determined by the direction of the flow streamlines.
Where C ds (r) is the solution of equation (6) subject to boundary conditions (7) and (8).
with I k (∙) being the modified Bessel function of the first class and of order k for k = 0, 1 …, and λ ∈ R. Notice also that the operator given by equation (B19), as well as, the boundary conditions (B20) and (B21) originate when eigenfunctions ϕ λ (r, θ) for the operator A λ = - ∇2 are supposed to have the form ϕ λ (r, θ) = R λ (r)ψ(θ). The function γ k (λ) given by equation (B22) is motivated by the requirement of equation (B15) of radial symmetry in the limiting case λ → 0 for D > 0 fixed.
and σ k given by equation (B18) .
We are indebted to Dr. Ernesto Franco Vizcaino for language editing. We are also grateful to Jose Maria Dominguez and Francisco Ponce for the art work.
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